BEAM FILTER, PARTICULARLY FOR X-RAYS, THAT DOES NOT CHANGE THE BEAM'S SPECTRAL COMPOSITION

Description

[0001] The invention relates to an X-ray device comprising a beam filter for insertion between an X-ray source and an X-ray detector. Moreover, it relates to a CT scanner comprising such an X-ray device.

[0002] The US 6 157 703 describes an X-ray filter realized as a copper or beryllium plate with a matrix of apertures. The apertures can selectively be shifted between positions of alignment or misalignment with respect to the holes of a collimator. In the case of a misalignment, the metal of the plate in front of the collimator holes attenuates an X-ray beam and removes particularly low-energy photons, thus "hardening" the spectrum of the beam.

[0003] US 2003/0190013 A1 describes a scattered ray removal grid that has an overall shape of constant spherical curvature. The scattered ray removal grid has radiation absorbing portions arrayed in a lattice configuration and radiation non-absorbing portions made of thermoplastic resin disposed between the radiation absorbing portions.

[0004] Based on this situation it was an object of the present invention to provide filtering means that can particularly be used in devices with spectrally resolved detection.

[0005] This objective is achieved by an X-ray device according to claim 1 and a CT scanner according to claim 9. Preferred embodiments are disclosed in the dependent claims.

[0006] The X-ray device according to the present invention comprises a beam filter which is located between an X-ray source and an X-ray detector. Moreover, the X-ray source shall have some spatial extension such that it cannot be approximated by a point source. It typically comprises a comparatively small radiation emitting area, for example the anode surface of an X-ray tube. The "detection area" corresponds to the sensitive area of the X-ray detector. The beam filter comprises a plurality of (first) absorbing bodies for masking in their working position (i.e. when being disposed between the X-ray source and the detection area) different fractions of the radiation emitting area of the X-ray source at different points on the detection area. This means that there are at least two points on the detection area from which the (spatially extended!) X-ray source is seen partially masked by the plurality of absorbing bodies and for which the fraction of the masked source area is different.

[0007] The described beam filter has the advantage that different points on the detection area will be reached by different intensities of the radiation that is emitted by the X-ray source because these points lie in half-shades of different degrees. The intensity distribution in the detection area can therefore precisely be adapted to the requirements of a particular application. If a patient shall for example be X-rayed, more intensity can be supplied to central regions of the patient's body than to peripheral regions.

[0008] In general, the absorbing bodies of the beam filter may have some transmittance for the radiation emitted by the X-ray source such that their masking is not total. In a preferred embodiment of the invention, the absorbing bodies comprise however a material that is highly absorbing over the whole spectrum of the radiation emitted by the X-ray source. Said material may particularly comprise materials with a high (mean) atomic number Z like molybdenum (Mo) or tungsten (W), which have a high absorption coefficient for X-rays. Other suited materials are gold (Au), lead (Pb), platinum (Pt), tantalum (Ta) and rhenium (Re). The absorbing bodies may consist completely or only partially of one of the mentioned materials, and it may of course also comprise a mixture (alloy) of several or all of these materials. The use of highly absorbing materials implies that masked points of the X-ray source will not shine through but actually remain dark. The intensity of radiation reaching a point on the detection area will then (approximately) only be determined by the geometry of the absorbing bodies, which can very precisely be adjusted. A further advantage is that the intensity reduction at some point of the detector area will not imply a modification of the spectrum of the radiation, because the complete spectrum is blended out for the masked zones of the X-ray source while the complete spectrum passes unaffectedly for the unmasked zones. This intensity adjustment without spectral modification is particularly useful in spectral CT applications that require a known, definite spectrum of the source radiation for a unique interpretation of the measurements.

[0009] The beam filter comprises a plurality of absorbing bodies that mask in their working position different fractions of the X-ray source area at different points of the detection area. Moreover, these absorbing bodies are shaped as absorbing sheets and arranged in a stack, wherein intermediate spaces separate neighboring sheets. Such a stack of absorbing sheets behaves similar to a jalousie with a plurality of lamellae that mask or conceal a light source. The absorbing sheets are preferably flat, though they may in general also assume other three-dimensional shapes. The shapes of the plurality of absorbing sheets correspond to quadrilaterals in which two opposite sides are bent with different bending radius, wherein the two opposite sides are bent with different bending radius such that the absorbing sheets comprise a minimal width in a direction normal to the opposite sides at a central position along the opposite sides.

[0010] The aforementioned intermediate spaces between neighboring absorbing sheets of the stack are preferably filled with a spacer material like a polymer, particularly a solid polymer, a foamed polymer, or a polymer glue. The spacer material provides stability and definite dimensions for the whole stack and allows to handle it as a compact block. The spacer material should have an attenuation coefficient for X-rays that is significantly lower than the attenuation coefficient of the material of the absorbing sheets. The attenuation coefficient of the spacer may for example be smaller than about 5%, preferably smaller than about 1 % of the attenuation coefficient of the absorbing sheets for (the whole spectrum of) the radiation emitted by the X-ray source.

[0011] In another preferred embodiment of the beam filter with absorbing sheets, the sheets lie in planes that intersect in at least one common point. If the X-ray source is arranged such that it comprises said intersection point, the emitted radiation will propagate substantially in the direction of the planes. The radiation will therefore impinge onto the absorbing sheets parallel to the sheet plane, which guarantees a high absorption efficiency. It should be noted that if the planes are exactly planar and intersect in two common points, they will inevitably intersect in a complete line.

[0012] The absorbing sheets have a varying width, wherein said width is measured in radial direction with respect to a given point. Said point is preferably a common intersection point of the planes in which the absorbing sheets lie, because this guarantees that a ray starting at the point will impinge onto the complete width of the corresponding absorbing sheet in its plane.

[0013] According to the present invention, the varying width of the absorbing sheets assumes a minimal value in a central region of the absorbing sheets. As will be explained with reference to the Figures, this will result in an intensity peak in a central region of the radiation passing through the beam filter, which is favorable for example in CT applications.

[0014] The absorbing sheets optionally have a varying thickness, wherein the thickness may vary between different points on the same absorbing sheet as well as between points on different absorbing sheets. The thickness of the absorbing sheets is a further parameter that can be tuned to establish a desired intensity profile across the detection area.

[0015] In a further development of the invention, the beam filter comprises a plurality of second absorbing bodies that are movable relative to a first plurality of absorbing bodies and arranged such that the first and the second pluralities of absorbing bodies are placed one behind the other in the direction of X-ray propagation. The first and second pluralities of absorbing bodies therefore have to be passed consecutively by X-rays emitted by the X-ray source. As the first and second pluralities of absorbing bodies can be moved with respect to each other, it is possible to selectively change the overlap between zones of the X-ray source that are masked by the first and the second pluralities of absorbing bodies, respectively, which in turn changes the overall masking degree. Thus the intensity distribution across the detection area can be changed comparatively simple by moving the second plurality of absorbing bodies with respect to the first plurality of absorbing bodies.

[0016] Further advantageous embodiments are defined in the dependent claims.

[0017] The invention further relates to a Computed Tomography (CT) scanner, that comprises a X-ray device of the kind described above. As was already explained, the beam filter can establish practically any desired intensity profile in an associated detection area with minimal or even no changes to the spectrum of the X-ray source. This is especially useful for spectral CT scanners as they require that the radiation passing through an X-rayed object has a known, definite spectrum.

[0018] These and other aspects of the invention will be apparent from and elucidated with reference to the embodiment(s) described hereinafter. These embodiments will be described by way of example with the help of the accompanying drawings in which:

Figure 1 shows in a perspective schematically an X-ray device with a beam filter according to the present invention;

Figure 2 illustrates the geometry of an embodiment of the invention comprising a beam filter with one stack of absorbing sheets;

Figure 3 shows a top view of the beam filter of Figure 2;

Figure 4 shows a section along the line IV-IV of Figure 3;

Figure 5 shows a section along the line V-V of Figure 3;

Figure 6 shows a preferred embodiment comprising a beam filter in a representation like that of Figures 4 and 5, said beam filter comprising two stacks of absorbing sheets;

Figure 7 shows the beam filter of Figure 6 when the stacks of absorbing sheets are shifted relative to each other.

[0019] Like reference numbers or numbers differing by integer multiples of 100 refer in the Figures to identical or similar components.

[0020] X-ray devices according to the present invention will in the following be described in particular with respect to an application in spectral CT scanners.

[0021] Spectral CT is a very promising technology which allows the discrimination of different elements in the body. In general, spectral CT is based on the fact that chemical elements show a distinct difference in the energy-dependence of the attenuation coefficient. In order to measure this energy dependence, some sort of energy discrimination is required on the detector side. Furthermore, the primary spectrum of radiation entering an object to be imaged has to cover a broad range of energies. One important part of spectral CT is the measurement of the photo-absorption contribution to the attenuation coefficient, which relies on the detection of rather low-energy photons.

[0022] For dose reduction purposes in contemporary CT scanners, so-called "bow-tie" filters can be used to adjust the photon flux along the fan direction to the shape of a patient, i.e. the larger thickness of the patient in the center requires a higher intensity there, while less intensity suffices for the decreasing thickness at the periphery of the body. Such a filter may be realized by a varying thickness of a light metal like Aluminum. The disadvantage of this approach for spectral CT is however that the filter will change the spectral shape of the primary radiation along the fan direction. Particularly the low-energy photons, which are of high importance for the measurement of the photo-absorption, are attenuated. As a consequence, this will reduce the possibility of spectral deconvolution in the edge regime of the fan, where the bow-tie filter exhibits its maximum thickness.

[0023] Due to these reasons there is a need for an alternative beam filter that allows to control the intensity profile of an X-ray beam, particularly a fan shaped beam, with minimal or ideally no modification of the radiation spectrum.

[0024] To achieve the aforementioned objective, it is proposed here to use a plurality of absorbing bodies that mask or conceal the X-ray source to different degrees as seen from different points of the detection area. Figure 1 illustrates the principal setup, which comprises a beam filter 10 located between a spatially extended X-ray source 1 (e.g. the anode area of an X-ray tube) and a detector area 2 (e.g. the scintillator material or direct conversion material of a digital X-ray detector). The beam filter 10 comprises a stack 100 of absorbing sheets 111 that are separated by intermediate spaces 112. X-rays X emitted by the X-ray source 1 will have to pass through the beam filter 10 before they can reach the detector area 2. Some of these rays will pass freely through the intermediate spaces 112 while others impinge on the absorbing sheets 111, where they are substantially completely absorbed. The attenuation of the X-ray beam is therefore realized by a "partial total absorption" of the radiation ("partial" with respect to the whole set of rays of the beam, "total" with respect to single absorbed rays), wherein the attenuated radiation basically preserves its initial spectral configuration.

[0025] Figure 1 illustrates this filtering principle by showing enlarged sketches of the images I_A and I_B with which the area of the radiation source 1 is seen from a central point A and a peripheral point B on the detection area 2, respectively. Due to the particular shape of the absorbing sheets 111, the zones M_A in which the radiation source I is masked in the central image I_A have a smaller total area than the zones M_B in which the radiation source 1 is masked in the peripheral image I_B. Consequently, the central point A will be illuminated with a higher beam intensity than the peripheral point B, as illustrated above the detection area in the profile of the intensity Φ along a line x through points A and B (it should be noted that the intensity profile will be balanced again if an object with a central thickness maximum, e.g. a patient, is placed between the beam filter 10 and the detection area 2). As the total radiation at the points A and B is composed in an all-or-nothing manner only of radiation that freely passed the beam filter 10 (and not or at least to only a minimal degree of radiation that passed an absorbing sheet), the spectral composition of the total radiation arriving at points A and B remains approximately the same.

[0026] Figure 2 illustrates the principal geometry of an embodiment comprising a beam filter 10 according to the present invention. This beam filter 10 consists of a stack 100 of absorbing sheets 111 of substantially the same shape, wherein said shape corresponds to a quadrilateral in which two opposite sides are bent with different bending radius (wherein the bending radius of the convex side is larger than that of the concave side). Each of the flat absorbing sheets 111 lies in a plain P, wherein all these planes P intersect in a common line L and therefore also in a common "focal point" F (lying also on the symmetry line of the absorbing sheets 111).

[0027] When the beam filter 10 is applied for example in an X-ray device like that of Figure 1, the radiation source 1 is located such that it comprises the aforementioned focal point F. Radiation emitted by the source 1 will then propagate approximately radially from the focal point F (not exactly for all rays, as the radiation source 1 is not a mathematical point but has some finite extension). An important aspect of the beam filter 10 is that the width of its absorbing sheets 111 as measures along radii r originating at the focal spot F is variable. As can best be seen in the top view of the stack 100 of absorbing sheets 111 shown in Figure 3, this width assumes a maximal value d_B at the periphery of the absorbing sheets 111 and declines continuously towards the centre of the absorbing sheets 111, where it assumes its minimal value d_A.

[0028] Figures 4 and 5 show sections along the lines IV-IV and V-V, respectively, of Figure 3. It can be seen that the beam filter 10 comprises a stack 100 of (in the example five) absorbing sheets 111 separated by (four) intermediate spacers 112 that are transparent for X-radiation and that may consist for example of a polymethacrylimide hard foam material (commercially available under the name Rohacell® from Degussa, Germany). The absorbing sheets 111 typically consist of a highly absorbing material, for example molybdenum or tungsten. Moreover, the absorbing sheets are focused towards the X-radiation source 1 due to their arrangement in planes P (Figure 2). As the Figures illustrate particularly for X-rays that propagate parallel to the central symmetry axis of the setup, a larger fraction of the radiation emitted by the radiation source 1 is absorbed in the peripheral part of the beam filter 10 where the absorbing sheets 11 1 have a high width d_B than in the central part where the absorbing sheets 111 have a short width d_A.

[0029] The described design of the beam filter 10 can be modified in various ways, for example by:

• changing the thickness (measured perpendicular to the sheet plane) of the highly absorbing sheets 111 relative to the thickness of the spacer sheets 112,
• tilting the whole stack 100,
• a suitable deformation of the absorbing sheets 111.

[0030] Figures 6 and 7 illustrate a second design of a beam filter 20 with adjustable absorbing properties, said beam filter 20 consisting of two stacks 100, 200 of absorbing sheets 111 and 211, respectively, wherein each of these stacks has a design like the beam filter 10 described above. The two stacks 100, 200 of absorbing sheets 111, 211 are placed one behind the other in the direction of the X-ray propagation. X-rays will therefore have to pass both stacks 100, 200 before they can reach a detector. The area of the X-radiation source 1 that is masked by the absorbing sheets 111, 211 can be changed if the stacks 100, 200 are shifted with respect to each other. Figure 6 shows in this respect an arrangement in which the absorbing sheets of the two stacks 100, 200 are aligned, while Figure 7 shows an arrangement in which the second stack 200 is shifted somewhat with respect to the first stack 100, resulting in a reduced intensity of the beam at the output side.

[0031] In the described embodiment comprising a primary beam filter with a multi-layer structure, the spectral shape of the radiation is hardly changed as attenuation is realized by partial total absorption. The beam filters are favorably applicable in medical CT, particularly spectral CT.

[0032] Finally it is pointed out that in the present application the term "comprising" does not exclude other elements or steps, that "a" or "an" does not exclude a plurality, and that a single processor or other unit may fulfill the functions of several means. The invention resides in each and every novel characteristic feature and each and every combination of characteristic features. Moreover, reference signs in the claims shall not be construed as limiting their scope.

Claims

1. An X-ray device, comprising:

- an X-ray source (1);

- an X-ray detector comprising a sensitive area (2) for detecting X-rays (X) emitted by the X-ray source (1);

- a beam filter (10; 20) located between the X-ray source (1) and the X-ray detector, the beam filter (10; 20) comprising a plurality of absorbing bodies (111; 211) for masking different fractions of a radiation emitting area of the X-ray source (1) at different points (A, B) of the sensitive area (2) of the X-ray detector, wherein the absorbing bodies are shaped as absorbing sheets (111; 211) and arranged with intermediate spaces (112) in a stack (100; 200) and wherein the shapes of the plurality of absorbing sheets correspond to quadrilaterals in which two opposite sides are bent with different bending radius, characterized in that the two opposite sides are bent with different bending radius such that the absorbing sheets comprise a minimal width (d_A) in a direction normal to the opposite sides at a central position along the opposite sides.

2. The X-ray device according to claim 1,
characterized in that the absorbing bodies (111; 211) comprise a material selected from the group consisting of Mo, W, Au, Pb, Pt, Ta and Re.

3. The X-ray device according to claim 1,
characterized in that the intermediate spaces are filled with a spacer material (112) which has a lower attenuation coefficient for the whole spectrum of the X-rays emitted by the X-ray source (1) than the material of the absorbing sheets, particularly a polymer.

4. The X-ray device according to claim 1,
characterized in that the absorbing sheets (111, 211) lie in planes (P) that intersect in at least one common point (F, L).

5. The X-ray device according to claim 1,
characterized in that the absorbing sheets (111, 211) have varying thicknesses.

6. The X-ray device according to claim 1,
characterized in that the beam filter (10; 20) comprises a plurality of second absorbing bodies (211) that are movable relative to a first plurality of absorbing bodies (111) and arranged such that the first (111) and the second (211) pluralities of absorbing bodies are placed one behind the other in the direction of X-ray propagation.

7. The X-ray device according to claim 1, characterized in that the two bent opposite sides define a convex side and a concave side, wherein the bending radius of the convex side is larger than that of the concave side.

8. A CT scanner comprising the X-ray device according to claim 1.

Ansprüche

1. Röntgenvorrichtung, die Folgendes umfasst:

- eine Röntgenquelle (1);

- einen Röntgendetektor mit einem empfindlichen Bereich (2) zum Detektieren der durch die Röntgenquelle (1) emittierten Röntgenstrahlen (X);

- einen zwischen der Röntgenquelle (1) und dem Röntgendetektor angeordneten Strahlungsfilter (10; 20), wobei der Strahlungsfilter (10; 20) eine Vielzahl von absorbierenden Körpern (111; 211) zum Maskieren unterschiedlicher Fraktionen eines Strahlung emittierenden Bereichs der Röntgenquelle (1) an verschiedenen Punkten (A, B) des empfindlichen Bereichs (2) des Röntgendetektors umfasst, wobei die absorbierenden Körper als absorbierende Blätter (111; 211) geformt sind und mit Zwischenräumen (112) in einem Stapel (100; 200) angeordnet sind, und wobei die Formen der Vielzahl von absorbierenden Blättern Vierecken entsprechen, in denen zwei gegenüberliegende Seiten mit unterschiedlichem Biegeradius gebogen sind,
dadurch gekennzeichnet, dass die beiden gegenüberliegenden Seiten mit einem unterschiedlichen Biegeradius so gebogen sind, dass die absorbierenden Blätter eine minimale Breite (d_A) in einer Richtung senkrecht zu den gegenüberliegenden Seiten bei einer mittleren Position entlang der gegenüberliegenden Seiten umfassen.

2. Röntgenvorrichtung nach Anspruch 1,
dadurch gekennzeichnet, dass die absorbierenden Körper (111; 211) ein Material ausgewählt aus der Gruppe bestehend aus Mo, W, Au, Pb, Pt, Ta und Re umfassen.

3. Röntgenvorrichtung nach Anspruch 1,
dadurch gekennzeichnet, dass die Zwischenräume mit einem Abstandsmaterial (112) gefüllt sind, welches einen geringeren Abschwächungskoeffizienten für das gesamte von der Röntgenquelle (1) emittierte Röntgenspektrum hat als das Material der absorbierenden Blätter, insbesondere ein Polymer.

4. Röntgenvorrichtung nach Anspruch 1,
dadurch gekennzeichnet, dass die absorbierenden Blätter (111, 211) in Ebenen (P) liegen, die sich an mindestens einem gemeinsamen Punkt (F, L) schneiden.

5. Röntgenvorrichtung nach Anspruch 1,
dadurch gekennzeichnet, dass die absorbierenden Blätter (111, 211) eine unterschiedliche Dicke haben.

6. Röntgenvorrichtung nach Anspruch 1,
dadurch gekennzeichnet, dass der Strahlungsfilter (10; 20) eine Vielzahl von zweiten absorbierenden Körpern (211) umfasst, die in Bezug auf eine erste Vielzahl von absorbierenden Körpern (111) beweglich sind und so angeordnet sind, dass die erste (111) und die zweite (211) Vielzahl von absorbierenden Körpern eine hinter der anderen in Richtung der Röntgenausbreitung platziert sind.

7. Röntgenvorrichtung nach Anspruch 1,
dadurch gekennzeichnet, dass die beiden gebogenen gegenüberliegenden Seiten eine konvexe und eine konkave Seite definieren, wobei der Biegeradius der konvexen Seite größer ist als der der konkaven Seite.

8. CT-Scanner mit der Röntgenvorrichtung nach Anspruch 1.

Revendications

1. Dispositif à rayons X, comprenant :

- une source de rayons X (1) ;

- un détecteur de rayons X comprenant une zone sensible (2) pour détecter des rayons X (X) émis par la source de rayons X (1) ;

- un filtre à faisceau (10 ; 20) situé derrière la source de rayons X (1) et le détecteur de rayons X, le filtre à faisceau (10 ; 20) comprenant une pluralité de corps absorbants (111, 211) pour masquer différentes fractions d'une zone émettant un rayonnement de la source de rayons X (1) en des points différents (A, B) de la zone sensible (2) du détecteur de rayons X, où les corps absorbants sont formés en feuilles absorbantes (111 ; 211) et agencées avec des espaces intermédiaires (112) en un empilement (100 ; 200) et/ou les formes de la pluralité de feuilles absorbantes correspondent à des quadrilatères dans lesquels deux côtés opposés sont courbés avec un rayon de courbure différent,
caractérisé en ce que les deux côtés opposés sont courbés avec un rayon de courbure différent de sorte que les feuilles absorbantes ont une largeur minimale (d_A) dans une direction normale aux côtés opposés en une position centrale le long des côtés opposés.

2. Dispositif à rayons X selon la revendication 1,
caractérisé en ce que les corps absorbants (111 ; 211) comprennent un matériau choisi dans le groupe constitué par Mo, W, Au, Pb, Pt, Ta et Re.

3. Dispositif à rayons X selon la revendication 1,
caractérisé en ce que les espaces intermédiaires sont remplis d'un matériau espaceur (112) qui présente un coefficient d'atténuation plus bas pour tout le spectre des rayons X émis par la source de rayons X (1) que le matériau des feuilles absorbantes, en particulier un polymère.

4. Dispositif à rayons X selon la revendication 1,
caractérisé en ce que les feuilles absorbantes (111, 211) reposent dans des plans (P) qui se coupent en au moins un point commun (F, L).

5. Dispositif à rayons X selon la revendication 1,
caractérisé en ce que les feuilles absorbantes (111, 211) ont des épaisseurs variables.

6. Dispositif à rayons X selon la revendication 1,
caractérisé en ce que le filtre à faisceau (10 ; 20) comprend une pluralité de seconds corps absorbants (211) qui sont mobiles par rapport à une première pluralité de corps absorbants (111) et agencés de sorte que les première (111) et seconde (211) pluralités de corps absorbants sont placées l'une derrière l'autre dans la direction de la propagation de rayons X.

7. Dispositif à rayons X selon la revendication 1,
caractérisé en ce que les deux côtés opposés courbés définissent un côté convexe et un côté concave, où le rayon de courbure du côté convexe est plus grand que celui du côté concave.

8. Tomodensitomètre comprenant le dispositif à rayons X selon la revendication 1.

Drawing